The decay of the X(3872) including \(J/\psi \pi ^+\pi ^-\)  and \(D^0\bar{D}^{*0}\)  and \(\bar{D}^0D^{*0}\)  final states are studied by BESIII, BABAR and BELLE [1]}, [2]}, [3]}, [4]}, [5]}, [6]}.
Furthermore, other \(X(3872)\)  decay channels that have been observed experimentally are
\(J/\psi \pi ^+\pi ^-\pi ^0\)  [7]},
\(J/\psi \gamma \)  [8]} and \(\psi ^{\prime }\gamma \)  [8]},
with relative branching ratios

\(\frac{Br(X\rightarrow J/\psi \pi ^+\pi ^-\pi ^0)}{Br(X\rightarrow J/\psi \pi ^+\pi ^-)}&=&1.0\pm 0.4\pm 0.3,\\\frac{Br(X\rightarrow J/\psi \gamma )}{Br(X\rightarrow J/\psi \pi ^+\pi ^-)}&=&0.33\pm 0.12,\\\frac{Br(X\rightarrow \psi ^{\prime }\gamma )}{Br(X\rightarrow J/\psi \pi ^+\pi ^-)}&=&1.1\pm 0.4.\) 
